Beat frequency- universal mathematical proof?

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Discussion Overview

The discussion revolves around the concept of beat frequency generated by the superposition of periodic waves, particularly focusing on the mathematical proof and insights applicable to various types of waves beyond just sinusoidal forms. Participants explore the conditions under which beats occur and the relationship between beats and amplitude modulation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants derive the beat frequency from trigonometric identities, specifically for cosine waves, and question the existence of a universal proof for all periodic waves.
  • Others argue that beats only occur when two waves are close in wavelength, while far apart wavelengths lead to amplitude modulation, suggesting a distinction between these phenomena.
  • A participant expresses skepticism about the general applicability of the cosine-cosine proof to all wave shapes, prompting discussions about the role of geometry and the nature of periodic functions.
  • There is mention of the ability to represent any periodic function as a linear sum of sinusoids, which some participants relate to Fourier series.
  • One participant discusses the transformation between beats and amplitude modulation, noting that while they are mathematically related, the physical phenomena differ due to the involvement of additional terms in amplitude modulation.
  • Several participants share personal experiences and insights from working with sound waves and radio, contributing to the understanding of these concepts.

Areas of Agreement / Disagreement

Participants express differing views on the conditions necessary for beat frequencies to occur and the relationship between beats and amplitude modulation. There is no consensus on a universal proof applicable to all periodic waves, and the discussion remains unresolved regarding the deeper understanding of these phenomena.

Contextual Notes

Some participants highlight the limitations of relying solely on trigonometric identities and emphasize the need for a broader understanding of the underlying principles governing wave interactions. The discussion also touches on the complexity of mathematical representations and their physical implications.

dunnoe
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It is easily derived from trigonometric identities that

cos(2*pi*f1*t)+cos(2*pi*f2*t)=2cos(2*pi*(f2+f1)*t)*cos(2*pi*(abs(f2-f1)*t))

which proves that superposition of two cosine wave will generate a beat frequency, but what about about a universal proof that applies to any kind of periodic waves.

Rather I am more curious about the insight behind why superposition of two frequency will generate a beat frequency.
 
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but what about about a universal proof that applies to any kind of periodic waves
That was it.
You don't always get beats though - that's just when the two waves are close in wavelength. Far apart in wavelength you get amplitude modulation and in-between you get a nasty looking ... thing.
Rather I am more curious about the insight behind why superposition of two frequency will generate a beat frequency.
srsly? do you also wonder how two lengths at an angle can make an area? It's geometry.
 
Simon Bridge said:
That was it.
You don't always get beats though - that's just when the two waves are close in wavelength. Far apart in wavelength you get amplitude modulation and in-between you get a nasty looking ... thing.
srsly? do you also wonder how two lengths at an angle can make an area? It's geometry.

At first, I was skeptical that two periodic waves which are close in wavelength regardless of their shape will generate a beat frequency given only proof of the cosine-cosine case. Later, I toyed with MATLAB and plotted sine-sine, cosine-cosine & sine-squarewave graph which showed beat frequency as well. Surely there's a reason beyond geometry it's applicable for waves of all shapes . I don't think being able to derive a formula is the same as understanding the formula.
 
You don't always get beats though - that's just when the two waves are close in wavelength. Far apart in wavelength you get amplitude modulation and in-between you get a nasty looking ... thing.

Are you sure about this?

There is a transformation between the sum and product of two sinusoids, one is called beats, the other is called amplitude modulation.

You might want to review the discussion in this recent thread.

https://www.physicsforums.com/showthread.php?t=567089
 
dunnoe said:
At first, I was skeptical that two periodic waves which are close in wavelength regardless of their shape will generate a beat frequency given only proof of the cosine-cosine case.
The reason you need only do the proof for the sinusoidal case is that every other periodic function can be expanded as a linear sum of sinusoids. Which is a separate proof.
Later, I toyed with MATLAB and plotted sine-sine, cosine-cosine & sine-squarewave graph which showed beat frequency as well. Surely there's a reason beyond geometry it's applicable for waves of all shapes .
Can you provide an example in math where there is a reason "beyond geometry" for something?

But you must realize that geometry is as basic as you can get.
eg. "Geometry, coeternal with God and shining in the divine Mind, gave God the pattern... by which he laid out the world so that it might be best and most beautiful and finally most like the Creator."
--- Johannes Kepler [1]

The effect you see is due to constructive and destructive interference - if the two waves have a different frequency then it follows that there must be a place where a trough of one must line up with a peak of the other and give you zero while at other places there must be two peaks or two troughs matching up and in-between you must get the, well, "in between" case.

What you are graphing is more: y=f(x).sin(kx) ... where f(x) happens to be another periodic with a different k. It doesn't have to be - all f(x) is doing is determining the amplitude of the sinusoid. Try f(x)=1/x for another famous example (you'll have to deal with what happens at x=0 though.).

You can also examine the case where the two waves have exactly the same frequency but different phases.

I don't think being able to derive a formula is the same as understanding the formula.
Well that's correct.

It's the trig ID that has you thrown off balance a bit?
It is a shortcut to actually doing the addition directly - with it's own separate proof.
One way of exploring underlying principles is to use the phasor representation for the waves - it's much more general.

---------------------------------------
[1] Quoted by Field J. V. in: Kepler's Geometrical Cosmology (1988), p. 123

quoted in Kepler's Geometrical Cosmology (1988), p. 123]
 
Studiot said:
Are you sure about this?
Quite sure :) worked with radio for ages.
There is a transformation between the sum and product of two sinusoids, one is called beats, the other is called amplitude modulation.
I know - these are two classes of the same math - and there is a continuous transform from one to the other.

It is easiest to demonstrate what I'm talking about when you try it with soundwaves that are audible - using a multivibrator you can change the relative frequencies continuously to move from beats to AM ... in between the two there is a horrible noise. The wave-form on an oscilloscope does not look like beating nor AM. That's what I was talking about.

What I was trying to get across was that multiplying two periodic waves does not always produce beats. It was not my intention to be specific about every possible result.

Hope that clears up any confusion.
 
Simon Bridge said:
The reason you need only do the proof for the sinusoidal case is that every other periodic function can be expanded as a linear sum of sinusoids. Which is a separate proof.

Thank you for the very satisfying response.

Wow, i never though of it in term of Fourier series.
Simon Bridge said:
Can you provide an example in math where there is a reason "beyond geometry" for something?

But you must realize that geometry is as basic as you can get.
eg. "Geometry, coeternal with God and shining in the divine Mind, gave God the pattern... by which he laid out the world so that it might be best and most beautiful and finally most like the Creator."
--- Johannes Kepler [1]

I admit that I have a poor understanding on the definition of geometry back then.

Simon Bridge said:
It's the trig ID that has you thrown off balance a bit?
Yup, definitely got confused by the trigonometry identity.
 
dunnoe said:
Thank you for the very satisfying response.
No worries - it helps to make links between different parts of your knowledge.

Hopefully you now have some of the deeper understanding you were after.
 
Originally Posted by Studiot
Are you sure about this?

Originally Posted by Simon Bridge

Quite sure :) worked with radio for ages.
There is a transformation between the sum and product of two sinusoids, one is called beats, the other is called amplitude modulation.

I know - these are two classes of the same math - and there is a continuous transform from one to the other.

The maths of the sum or product of sinusoids is as you say, classes or opposite sides of the same equation.

However the relationship of the physical phenomena of beats and amplitude modulation is not quite the same.

This is because there is an extra term in the maths for amplitude modulation that does not appear in the trigonometric transformation or beat frequency derivation discussed above.

This results in there being two frequencies ( at any stage) only being involved in the sum or product but three in amplitude modulation.
 

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